Optical fiber

ABSTRACT

An optical fiber includes a glass fiber and a coating resin covering an outer periphery of the glass fiber. The glass fiber includes a core and a cladding. An outer diameter of the glass fiber is 99 μm or larger and 101 μm or smaller. The coating resin includes a cured material of an ultraviolet curing resin composition. An outer diameter of the coating resin is 160 μm or larger and 170 μm or smaller. A mode field diameter for light having a wavelength of 1310 nm is 7.2 μm or larger and 8.2 μm or smaller. Bending loss at a wavelength of 1550 nm when wound in a ring shape having a radius of 10 mm is 0.1 dB/turn or less. Bending loss at the wavelength of 1550 nm when wound in the ring shape having the radius of 7.5 mm is 0.5 dB/turn or less.

CROSS REFERENCE

The present application is based upon and claims the benefit of thepriority from Japanese patent application No. P2019-035767, filed onFeb. 28, 2019, which is hereby incorporated by reference in itsentirety.

TECHNICAL FIELD

The present disclosure relates to an optical fiber.

BACKGROUND

JPH05-60954A discloses an optical fiber core wire having an outerdiameter of 230 μm or smaller and provided with an optical fiber made ofquartz glass and having an outer diameter of 125 μm and a coating formedof a resin. In the optical fiber core wire, a diameter is reduced bythinning a coating thickness.

SUMMARY

An optical fiber according to one embodiment of the present disclosureincludes a glass fiber and a coating resin covering an outer peripheryof the glass fiber. The glass fiber includes a core and a claddingcovering an outer periphery of the core. A refractive index of thecladding is lower than a refractive index of the core. An outer diameterof the glass fiber is 99 μm or larger and 101 μm or smaller. The coatingresin includes a cured material of an ultraviolet curing resincomposition. An outer diameter of the coating resin is 160 μm or largerand 170 μm or smaller. A mode field diameter for light having awavelength of 1310 nm is 7.2 μm or larger and 8.2 μm or smaller. Bendingloss at a wavelength of 1550 nm when wound in a ring shape having aradius of 10 mm is 0.1 dB/turn or less. Bending loss at the wavelengthof 1550 nm when wound in the ring shape having the radius of 7.5 mm is0.5 dB/turn or less.

BRIEF DESCRIPTION OF THE DRAWINGS

The foregoing and other purposes, aspects and advantages will be betterunderstood from the following detailed description of a preferredembodiment of the invention with reference to the drawings, in which:

FIG. 1 illustrates a sectional view and a refractive index distributionof an optical fiber according to one embodiment; and

FIG. 2 illustrates a sectional view and a refractive index distributionof an optical fiber according to a modification.

DETAILED DESCRIPTION Problem to be Solved by the Present Disclosure

In the optical fiber core wire described above, the coating resinthickness is thin. Therefore, when the optical fiber core wire isdensely housed in a cable, irregular stress applied to a coating resinas a lateral pressure is easily transmitted to an optical fiber. Thus,the optical fiber is irregularly bent and there is a risk thattransmission loss referred to as microbending loss increases.

Then, an object is to provide an optical fiber capable of suppressingthe transmission loss while reducing a diameter.

Advantageous Effect of the Present Disclosure

According to the present disclosure, the optical fiber capable ofsuppressing the transmission loss while reducing the diameter can beprovided.

Description of Embodiments of the Present Disclosure

First, embodiments of the present disclosure will be listed anddescribed. The optical fiber according to one embodiment of the presentdisclosure includes a glass fiber and a coating resin covering an outerperiphery of the glass fiber. The glass fiber includes a core and acladding covering an outer periphery of the core. A refractive index ofthe cladding is lower than a refractive index of the core. An outerdiameter of the glass fiber is 99 μm or larger and 101 μm or smaller.The coating resin includes a cured material of an ultraviolet curingresin composition. An outer diameter of the coating resin is 160 μm orlarger and 170 μm or smaller. A mode field diameter for light having awavelength of 1310 nm is 7.2 μm or larger and 8.2 μm or smaller. Bendingloss at a wavelength of 1550 nm when wound in a ring shape having aradius of 10 mm is 0.1 dB/turn or less. Bending loss at the wavelengthof 1550 nm when wound in the ring shape having the radius of 7.5 mm is0.5 dB/turn or less.

In the optical fiber according to the embodiment described above, theouter diameter of the glass fiber is 99 μm or larger and 101 μm orsmaller. Therefore, even when the outer diameter of the coating resin is160 μm or larger and 170 μm or smaller and the diameter is reduced, athickness of the coating resin is secured. Thus, even in a case whereirregular stress is applied to the coating resin as a lateral pressure,irregular bending of the glass fiber is suppressed. In addition, sincethe mode field diameter is reduced, confinement of light isstrengthened. Thus, microbending loss is suppressed. Therefore,transmission loss can be suppressed while reducing the diameter.

In one embodiment, a cable cutoff wavelength may be 1530 nm or shorter.Transmission loss at the wavelength of 1530 nm or longer and 1565 nm orshorter may be 0.3 dB/km or less. A loss increase amount at thewavelength of 1550 nm when an outer periphery of a cylinder having theouter diameter of 280 mm is covered with sandpaper of #240 and theoptical fiber is wound around the outer periphery of the cylinder withtension of 0.8 N in such a way as to be in contact with the sandpapermay be 1 dB/km or less. In this case, the light having the wavelength of1550 nm can be transmitted with low loss.

In one embodiment, a cable cutoff wavelength may be 1260 nm or shorter.Transmission loss at the wavelength of 1310 nm or longer and 1625 nm orshorter may be 0.4 dB/km or less. A loss increase amount at thewavelength of 1550 nm when an outer periphery of a cylinder having theouter diameter of 280 mm is covered with sandpaper of #240 and theoptical fiber is wound around the outer periphery of the cylinder withtension of 0.8 N in such a way as to be in contact with the sandpapermay be 1 dB/km or less. In this case, the light having the wavelength of1550 nm can be transmitted with low loss.

In one embodiment, a MAC value being a ratio of a mode field diameterMFD [μm] for the light having the wavelength of 1310 nm to a cablecutoff wavelength λcc [nm] may be 6.9 or smaller. In this case, themicrobending loss can be more surely suppressed.

In one embodiment, a virtual temperature of glass configuring the glassfiber may be 1600° C. or higher and 1700° C. or lower. In this case,since increase of the virtual temperature is suppressed, the increase ofthe transmission loss correlated with the virtual temperature issuppressed.

In one embodiment, the core may include a material in which germanium isadded to pure silica glass. The cladding may include the pure silicaglass. The cladding may have an absorption peak at a wave number of 2500cm⁻¹ or larger and 3000 cm⁻¹ or smaller in an IR spectrum. In this case,since the germanium is added to the core, a specific refractive indexdifference between the core and the cladding can be turned to apredetermined value or larger. In addition, the cladding has theabsorption peak due to deuterium processing. That is, since defectsincreased accompanying diameter reduction of the glass fiber arerepaired by the deuterium processing, the transmission loss can besuppressed further.

In one embodiment, tensile strength in a center axis direction may belarger than 0.69 GPa. In this case, disconnection of the optical fibercan be suppressed.

In one embodiment, the coating resin may include a primary coating resinlayer covering the outer periphery of the glass fiber and a secondarycoating resin layer covering an outer periphery of the primary coatingresin layer. In this case, a microbending loss resistant characteristiccan be efficiently improved.

In one embodiment, a Young's modulus of the primary coating resin layermay be 0.7 MPa or smaller. An outer diameter of the primary coatingresin layer may be 120 μm or larger and 140 μm or smaller. A Young'smodulus of the secondary coating resin layer may be 800 MPa or largerand 3000 MPa or smaller. An outer diameter of the secondary coatingresin layer may be 150 μm or larger and 170 μm or smaller. In this case,the microbending loss resistant characteristic can be efficientlyimproved.

In one embodiment, the coating resin may further include a colored resinlayer covering an outer periphery of the secondary coating resin layer.An outer diameter of the colored resin layer may be 160 μm or larger and170 μm or smaller. In this case, identification of the optical fiber isfacilitated by the colored resin layer.

In one embodiment, the secondary coating resin layer may includecoloring ink, and may configure an outermost layer of the coating resin.In this case, the identification of the optical fiber is facilitated bythe secondary coating resin layer.

Detailed Description of the Embodiments of the Present Disclosure

Specific examples of the optical fiber of the present disclosure will bedescribed with reference to drawings hereinafter. In description of thedrawings, same signs are attached to same elements and redundantdescription is omitted. Note that the present invention is not limitedto the examples and is indicated by the scope of claims, and it isintended to include meanings equal to the scope of the claims and allchanges within the scope.

FIG. 1 is a sectional view of the optical fiber according to oneembodiment and a diagram illustrating a refractive index distribution.As illustrated in FIG. 1, an optical fiber 1 of the present embodimentincludes a glass fiber 10 and a coating resin 20 covering the outerperiphery of the glass fiber 10. The sectional view in FIG. 1 expressesa cross section vertical to a center axis direction (optical axisdirection) of the optical fiber 1. The ordinate of the refractive indexdistribution in FIG. 1 indicates a refractive index.

The glass fiber 10 is a light guiding optical transmission body thattransmits light introduced to the optical fiber 1. The glass fiber 10 isa member made of glass, and is configured with silica (SiO₂) glass as abase material (main component) for example. A virtual temperature of theglass configuring the glass fiber 10 is 1600° C. or higher and 1700° C.or lower. An outer diameter (diameter) of the glass fiber 10 is 99 μm orlarger and 101 μm or smaller, and is smaller than the outer diameter(125 μm) of a general glass fiber. The glass fiber 10 includes a core 12extending along a predetermined axis, and a cladding 14 covering theouter periphery of the core 12. The core 12 and the cladding 14 areconcentrically arranged. The core 12 is provided in an area including acenter axis line of the glass fiber 10 for example. An outer diameter 2a of the core 12 is, for example, 5 μm or larger and 9 μm or smaller.The cladding 14 is provided in an area surrounding the core 12. Thecladding 14 is in contact with the outer periphery of the core 12. Anouter diameter of the cladding 14 is equal to the outer diameter of theglass fiber 10, and is 99 m or larger and 101 μm or smaller.

The core 12 and the cladding 14 are configured with the silica glass asthe base material (main component) for example. The core 12 includes amaterial in which germanium (Ge) is added to pure silica glass forexample. Here, the pure silica glass does not practically includeimpurities. The core 12 may include GeO₂ and/or elemental fluorine. Incontrast, the cladding 14 includes the pure silica glass for example.Thus, a refractive index n2 of the cladding 14 becomes lower than arefractive index n1 of the core 12, and a specific refractive indexdifference Δn between the core 12 and the cladding 14 can be turned to apredetermined value or larger.

The coating resin 20 includes a primary resin layer 22 (primary coatingresin layer) covering the outer periphery of the glass fiber 10, asecondary resin layer 24 (secondary coating resin layer) covering theouter periphery of the primary resin layer 22, and a colored resin layer26 covering the outer periphery of the secondary resin layer 24. Theglass fiber 10, the primary resin layer 22, the secondary resin layer 24and the colored resin layer 26 are concentrically arranged.

The primary resin layer 22 is in contact with an outer peripheralsurface of the cladding 14, and covers the whole cladding 14. A Young'smodulus of the primary resin layer 22 is, for example, 0.7 MPa orsmaller. The outer diameter of the primary resin layer 22 is, forexample, 120 μm or larger and 140 μm or smaller.

The secondary resin layer 24 is in contact with the outer peripheralsurface of the primary resin layer 22, and covers the whole primaryresin layer 22. The Young's modulus of the secondary resin layer 24 is,for example, 800 MPa or larger and 3000 MPa or smaller. The outerdiameter of the secondary resin layer 24 is, for example, 150 μm orlarger and 170 μm or smaller.

The primary resin layer 22 and the secondary resin layer 24 include acured material of an ultraviolet curing resin composition. That is, thecoating resin 20 includes the cured material of the ultraviolet curingresin composition. The ultraviolet curing resin composition used in theprimary resin layer 22 and the secondary resin layer 24 is urethaneacrylate for example. By applying the rein composition to the glassfiber 10, then radiating ultraviolet rays and causing the resincomposition to be cured, the primary resin layer 22 and the secondaryresin layer 24 are formed.

The colored resin layer 26 is in contact with the outer peripheralsurface of the secondary resin layer 24, and covers the whole secondaryresin layer 24. The colored resin layer 26 configures an outermost layerof the coating resin 20. The outer diameter of the coating resin 20 is160 μm or larger and 170 μm or smaller for example. The colored resinlayer 26 includes the cured material of the resin composition includingcoloring ink.

In the optical fiber 1 of the present embodiment, for example, the outerdiameter of the glass fiber 10 is 100 μm, the outer diameter of theprimary resin layer 22 is 135 μm, the outer diameter of the secondaryresin layer 24 is 155 μm, and the outer diameter of the colored resinlayer 26 is 165 μm.

One example of a manufacturing method of the optical fiber 1 will bedescribed. First, an optical fiber base material is prepared, and aglass fiber is formed by drawing the optical fiber base material. Thestep includes a step of gradually cooling the glass fiber drawn in adrawing furnace in a heating furnace at a temperature lower than thedrawing furnace, and a step (deuterium (D₂) processing) of exposing thegradually cooled glass fiber to a deuterium gas atmosphere. Note thatthe step of the deuterium processing may not be executed in a series ofdrawing step and may be executed in a different step after drawing isended.

First, the optical fiber base material is put into the drawing furnace,heated and melted, and the glass fiber turned to a small diameter ispulled out from the drawing furnace. Thereafter, gradual cooling isperformed in the heating furnace at the temperature lower than thedrawing furnace, and when glass is cured to a certain extent, forciblecooling is performed to be close to a room temperature.

When a cooling speed after drawing is accelerated by diameter reductionof the glass fiber, non-bridging oxygen hole centers (NBOHC) increase inthe glass fiber. The NBOHC is bonded with hydrogen and Si—OH isgenerated. When a hydroxyl group (—OH) is generated, transmission lossof the optical fiber 1 increases. By the D₂ processing, the NBOHC reactswith deuterium, and a deuterioxyl group (—OD) is generated. Since anabsorption peak of the deuterioxyl group is different from theabsorption peak of the hydroxyl group, increase of the transmission lossdue to the diameter reduction of the glass fiber can be suppressed. Thecladding of the D₂-processed optical fiber has the absorption peak at awave number of 2500 cm⁻¹ or larger and 3000 cm⁻¹ or smaller as theabsorption peak due to Si-OD, in an IR spectrum (infrared absorptionspectrum in infrared spectroscopy). Note that the IR spectrum can bemeasured by a general measuring apparatus such as ThermoScientificNicolet 8700 made by ThermoFisher Scientific.

Next, a layer to be the primary resin layer 22 is formed by applying theultraviolet curing resin composition on a surface of the formed glassfiber, and a layer to be the secondary resin layer 24 is formed byapplying the ultraviolet curing resin composition on the surface of thelayer. Then, the layers are cured by ultraviolet irradiation, and theprimary resin layer 22 and the secondary resin layer 24 are formed. Notethat an applying method is not limited to the above description, and theprimary resin layer may be applied, then irradiated with ultravioletrays and cured and the secondary resin layer may be applied and curedthereafter. In this method, first, the layer to be the primary resinlayer 22 is formed by applying the ultraviolet curing resin compositionand is cured by the ultraviolet irradiation to form the primary resinlayer 22. Then, the layer to be the secondary resin layer 24 is formedby applying the ultraviolet curing resin composition on the surface ofthe primary resin layer 22 and is cured by the ultraviolet irradiationto form the secondary resin layer 24.

Next, the colored resin layer 26 is formed on the surface of thesecondary resin layer 24, and the optical fiber is obtained. Note thatthe colored resin layer may be formed in a step different from thedrawing step.

Subsequently, a screening test is executed to the obtained opticalfiber. In the screening test, the optical fiber is pulled by 0.69 GPa inthe center axis direction, and tensile strain of 1% is generated. Forexample, when there is a scratch on the surface of the glass fiber, theoptical fiber is disconnected at the part. The part which is notdisconnected by the screening test, that is, the part where the tensilestrength in the center axis direction is larger than 0.69 GPa, isdefined as the optical fiber 1.

In the optical fiber 1 obtained as above, the outer diameter of theglass fiber 10 is 99 μm or larger and 101 μm or smaller. Therefore, evenwhen the outer diameter of the coating resin 20 is 160 μm or larger and170 μm or smaller and the diameter is reduced, a thickness of thecoating resin 20 is secured. Thus, even in a case where irregular stressis applied to the coating resin 20 as a lateral pressure, irregularbending of the glass fiber 10 is suppressed. In addition, in the opticalfiber 1, a mode field diameter for light having a wavelength of 1310 nmis 7.2 μm or larger and 8.2 μm or smaller and is narrowed around 7.7 μm.Thus, microbending loss is suppressed. Therefore, the transmission losscan be suppressed while reducing the diameter. Note that the mode fielddiameter is according to a definition of Petermann-I.

As described above, the primary resin layer 22 and the secondary resinlayer 24 are formed by applying the resin composition on the surface ofthe drawn glass fiber 10 and curing the resin composition. When thethickness of the primary resin layer 22 and the secondary resin layer 24is thin, there is a case where the resin composition cannot follow theglass fiber when the glass fiber is drawn at a high linear velocity andso-called application shortage occurs. In the optical fiber 1, since thethickness of the coating resin 20 is secured, the application shortageis suppressed. Thus, the optical fiber 1 can be stably manufactured.

In the screening test described above, the optical fiber is stronglyclamped by a roller and a capstan belt. At the time, when a solidforeign matter is stuck to the surface of the optical fiber, there is arisk that the foreign matter breaks through a resin coating film and thesurface of the glass fiber is scratched, causing disconnection. Theoptical fiber 1 is normally shipped by a fixed length (specifiedlength). When a disconnection frequency increases, the optical fiber 1of a fractional length which is shorter than the specified length andcannot be shipped increases. Thus, a yield declines and a manufacturingcost increases. In the optical fiber 1, since the thickness of thecoating resin 20 is secured, generation of a scratch on the surface ofthe glass fiber by the foreign matter is suppressed. As a result, sincethe disconnection is suppressed and the yield of the optical fiber 1improves, the manufacturing cost can be suppressed.

When the optical fiber 1 is wound around a mandrel having a radius of 10mm, that is, when the optical fiber 1 is wound in a ring shape havingthe radius of 10 mm, bending loss at the wavelength of 1550 nm is 0.1dB/turn or less. In addition, when the optical fiber 1 is wound aroundthe mandrel having the radius of 7.5 mm, that is, when the optical fiber1 is wound in the ring shape having the radius of 7.5 mm, the bendingloss at the wavelength of 1550 nm is 0.5 dB/turn or less.

A cable cutoff wavelength of the optical fiber 1 is 1530 nm or shorter.The transmission loss of the optical fiber 1 at the wavelength of 1530nm or longer and 1565 nm or shorter is 0.3 dB/km or less. A lossincrease amount (sandpaper lateral pressure loss increase) at thewavelength of 1550 nm when the outer periphery of a bobbin (cylinder)having the outer diameter of 280 mm is covered with sandpaper of #240and the optical fiber 1 is wound around the outer periphery of thebobbin with tension of 0.8 N in such a way as to be in contact with thesandpaper is 1 dB/km or less. Thus, by the optical fiber 1, the lighthaving the wavelength of 1550 nm can be transmitted with low loss. Sincethe wavelength 1550 nm is generally and widely used, it is not needed toexchange an existing transmitter-receiver, and a communication networkcan be constructed at a low cost.

Or, the cable cutoff wavelength of the optical fiber 1 is 1260 nm orshorter. The transmission loss of the optical fiber 1 at the wavelengthof 1310 nm or longer and 1625 nm or shorter is 0.4 dB/km or less. Theloss increase amount at the wavelength of 1310 nm when the outerperiphery of the bobbin (cylinder) having the outer diameter of 280 mmis covered with the sandpaper of #240 and the optical fiber 1 is woundaround the outer periphery of the bobbin with tension of 0.8 N in such away as to be in contact with the sandpaper is 1 dB/km or less. Thus, bythe optical fiber 1, the light having the wavelength of 1310 nm can betransmitted with low loss. Since the wavelength 1310 nm is generally andwidely used, it is not needed to exchange an existingtransmitter-receiver, and a communication network can be constructed ata low cost.

In the optical fiber 1, a MAC value (=MFD/λcc×1000) being a ratio of amode field diameter MFD [μm] for the light having the wavelength of 1310nm to a cable cutoff wavelength λcc [nm] is 6.9 or smaller. The MACvalue is correlated with the microbending loss, and the microbendingloss is suppressed when the MAC value is smaller. Thus, by the opticalfiber 1, the microbending loss can be more surely suppressed. An upperlimit value of the mode field diameter MFD for the light having thewavelength of 1310 nm is 8.1 μm for example. A lower limit value of thecable cutoff wavelength λcc is 1180 nm for example.

Since the cooling speed after the drawing is accelerated by the diameterreduction of the glass fiber 10, the drawing at the high linear velocitybecomes possible, and productivity improves. When the cooling speedafter the drawing is accelerated, the virtual temperature becomes high.The virtual temperature is correlated with the transmission loss, andthe transmission loss is suppressed when the virtual temperature islower. In the optical fiber 1, the virtual temperature of the glassconfiguring the glass fiber 10 is 1600° C. or higher and 1700° C. orlower. In this way, in the optical fiber 1, since the increase of thevirtual temperature is suppressed, the increase of the transmission lossis suppressed.

It is known that the virtual temperature can be measured by Ramanspectroscopy. In this method, a laser beam at the wavelength of 532 nmis converged to a fiber end face and a frequency spectrum of generatedRaman scattering light is measured. From the measured spectrum, an arearatio (D2/ω3) of a wide ω3 peak (800 cm⁻¹) due to Si—O—Si deformationvibrations intrinsic to quartz glass and a D2 peak (605 cm⁻¹) due tostretching vibrations of a three-membered ring is calculated. It isknown that there is a linear correlation between the calculated D2/ω3and the virtual temperature of the glass. Thus, the virtual temperatureof the fiber can be obtained from the correlation.

In the optical fiber 1, since the germanium is added to the core 12, thespecific refractive index difference between the core 12 and thecladding 14 can be turned to the predetermined value or larger. In thisway, since the core 12 includes the material in which the germanium isadded to the pure silica glass and the cladding 14 includes the puresilica glass, the optical fiber 1 can be manufactured by samemanufacturing facility and manufacturing process as a conventionalgeneral purpose single mode optical fiber. Thus, an initial cost can besuppressed.

In the optical fiber 1, in the IR spectrum, the cladding 14 has theabsorption peak at the wave number of 2500 cm⁻¹ or larger and 3000 cm⁻¹or smaller as the absorption peak due to the deuterium processing. Thus,the defects (NBOHC) increased accompanying the diameter reduction of theglass fiber 10 are repaired by the deuterium processing. Thus, thetransmission loss can be suppressed further.

Since the optical fiber 1 is manufactured through the screening test ofpulling by 0.69 GPa in the center axis direction, the tensile strengthin the center axis direction of the optical fiber 1 is larger than 0.69GPa. Thus, the disconnection of the optical fiber 1 can be suppressed.

The coating resin 20 includes the primary resin layer 22 and thesecondary resin layer 24. Therefore, for example, by configuring theprimary resin layer 22 by the material of the low Young's modulus andconfiguring the secondary resin layer 24 by the material of the highYoung's modulus or the like, a microbending loss resistantcharacteristic can be efficiently improved.

The Young's modulus of the primary resin layer 22 is 0.7 MPa or smaller.The outer diameter of the primary resin layer 22 is 120 μm or larger and140 μm or smaller. The Young's modulus of the secondary resin layer 24is 800 MPa or larger and 3000 MPa or smaller. The outer diameter of thesecondary resin layer 24 is 150 μm or larger and 170 μm or smaller.Thus, the microbending loss resistant characteristic can be efficientlyimproved.

Since the coating resin 20 includes the colored resin layer 26,identification of the optical fiber 1 is facilitated by the coloredresin layer 26. Note that, when the colored resin layer 26 is formed inthe drawing step, the step of forming the colored resin layer 26 can beomitted so that the productivity improves.

The present invention is not limited to the embodiment described aboveand can be variously modified.

FIG. 2 is a sectional view of the optical fiber according to amodification and a diagram illustrating a refractive index distribution.As illustrated in FIG. 2, an optical fiber 1A according to themodification is different from the optical fiber 1 according to theembodiment at a point of not including the colored resin layer 26 andincluding a secondary resin layer 24A instead of the secondary resinlayer 24. The secondary resin layer 24A is different from the secondaryresin layer 24 at the point of including coloring ink and configuringthe outermost layer of the coating resin 20. In the optical fiber 1A,for example, the outer diameter of the glass fiber 10 is 100 pun, theouter diameter of the primary resin layer 22 is 135 μm, and the outerdiameter of the secondary resin layer 24A is 165 μm.

Examples

The present invention will be more specifically described with exampleshereinafter, however, the present invention is not limited by theexamples described below.

Elements and characteristics of the optical fiber according to examples1 to 4 and a comparative example are indicated in Table 1.

TABLE 1 Example 1 Example 2 Example 3 Example 4 Comparative example Corecomposition Germanium-added quartz Cladding composition Pure quartzTransmission wavelength [nm] 1550 1550 1310 1310 1550 Core diameter (2a)[μm] 8.0 8.0 7.0 7.0 8.0 Cladding diameter [μm] 100 100 100 100 125Specific refractive index difference (Δn) [%] 0.55 0.55 0.48 0.48 0.55Primary resin layer Young's modulus [MPa] 0.7 0.7 0.7 0.7 0.7 Secondaryresin layer Young's modulus [MPa] 1000 1000 1000 1000 1000 Primary resinlayer outer diameter [μm] 135 135 135 135 140 Secondary resin layerouter diameter [μm] 155 165 155 165 165 Colored resin layer outerdiameter [μm] 165 None 165 None None MFD (1310 nm) [μm] 7.7 7.7 7.6 7.67.7 Cable cutoff wavelength [nm] 1462 1462 1203 1203 1462 MAC value 5.275.27 6.32 6.32 5.27 Bending loss (R 10 mm/1550 nm) [dB/turn] Less LessLess Less Less than 0.01 than 0.01 than 0.01 than 0.01 than 0.01 Bendingloss (R 7.5 mm/1550 nm) [dB/turn] Less Less Less Less Less than 0.01than 0.01 than 0.01 than 0.01 than 0.01 Sandpaper lateral pressure lossincrease 0.5 0.5 0.7 0.7 2.5 (1310 nm) [dB/km] Sandpaper lateralpressure loss increase 0.8 0.8 0.9 0.9 5.8 (1550 nm) [dB/km]Transmission loss (1310 nm) [dB/km] 0.33 0.33 0.35 0.35 0.33Transmission loss (1550 nm) [dB/km] 0.21 0.21 0.22 0.22 0.20 0.69 GPaScreening disconnection Less Less Less Less 12 frequency [times/km] than0.01 than 0.01 than 0.01 than 0.01

The optical fibers according to the examples 1 and 3 have a formcorresponding to the optical fiber 1 according to the embodimentdescribed above. The optical fibers according to the examples 2 and 4have a form corresponding to the optical fiber 1A according to themodification described above. The optical fiber according to thecomparative example has a form that the colored resin layer is notincluded and the secondary resin layer includes the coloring ink andconfigures the outermost layer of the coating resin, similarly to theoptical fiber 1A according to the modification described above.

As indicated in Table 1, in the optical fiber according to thecomparative example, the outer diameter (cladding diameter) of the glassfiber is 125 μm and the outer diameter (secondary resin layer outerdiameter) of the coating resin is 165 μm. Thus, the thickness of thecoating resin in the optical fiber according to the comparative exampleis roughly 20 μm. In contrast, in the optical fibers according to theexamples 1 to 4, the outer diameter (cladding diameter) of the glassfiber is 100 μm and the outer diameter (colored resin layer outerdiameter or secondary resin layer outer diameter) of the coating resinis 165 μm. Thus, the thickness of the coating resin in the opticalfibers according to the examples 1 to 4 is roughly 32.5 μm and isthicker than the thickness of the coating resin in the optical fiberaccording to the comparative example.

In the optical fiber according to the comparative example, the sandpaperlateral pressure loss increase at the wavelength of 1310 nm (the lossincrease amount at the wavelength of 1310 nm when the outer periphery ofthe bobbin having the outer diameter of 280 mm is covered with thesandpaper of #240 and the optical fiber 1 is wound around the outerperiphery of the bobbin with the tension of 0.8 N in such a way as to bein contact with the sandpaper) was 2.5 dB/km, and the loss increaseamount at the wavelength of 1550 nm was 5.8 dB/km. In contrast, in theoptical fibers according to the examples 1 to 4, the sandpaper lateralpressure increases at the wavelength of 1310 nm and the wavelength of1550 nm were both 1 dB/km or less.

In the optical fiber according to the comparative example, thedisconnection frequency of the optical fiber in the screening test ofpulling the optical fiber by 0.69 GPa in the center axis direction andgenerating the tensile strain of 1% was 12 times/km. In contrast, in theoptical fibers according to the examples 1 to 4, the disconnectionfrequencies of the optical fibers in the screening test were all lessthan 0.01 times/km.

In this way, compared to the optical fiber according to the comparativeexample, in the optical fibers according to the examples 1 to 4, sincethe thickness of the coating resin is secured, the sandpaper lateralpressure loss increase and the disconnection frequency in the screeningtest were suppressed.

What is claimed is:
 1. An optical fiber comprising a glass fiber and acoating resin covering an outer periphery of the glass fiber, whereinthe glass fiber includes a core and a cladding covering an outerperiphery of the core, a refractive index of the cladding is lower thana refractive index of the core, an outer diameter of the glass fiber is99 μm or larger and 101 μm or smaller, the coating resin includes acured material of an ultraviolet curing resin composition, an outerdiameter of the coating resin is 160 μm or larger and 170 μm or smaller,a mode field diameter for light having a wavelength of 1310 nm is 7.2 μmor larger and 8.2 μm or smaller, bending loss at a wavelength of 1550 nmwhen wound in a ring shape having a radius of 10 mm is 0.1 dB/turn orless, and bending loss at the wavelength of 1550 nm when wound in thering shape having the radius of 7.5 mm is 0.5 dB/turn or less.
 2. Theoptical fiber according to claim 1, wherein a cable cutoff wavelength is1530 nm or shorter, transmission loss at the wavelength of 1530 nm orlonger and 1565 nm or shorter is 0.3 dB/km or less, and a loss increaseamount at the wavelength of 1550 nm when an outer periphery of acylinder having the outer diameter of 280 mm is covered with sandpaperof #240 and the optical fiber is wound around the outer periphery of thecylinder with tension of 0.8 N in such a way as to be in contact withthe sandpaper is 1 dB/km or less.
 3. The optical fiber according toclaim 1, wherein a cable cutoff wavelength is 1260 nm or shorter,transmission loss at the wavelength of 1310 nm or longer and 1625 nm orshorter is 0.4 dB/km or less, and a loss increase amount at thewavelength of 1550 nm when an outer periphery of a cylinder having theouter diameter of 280 mm is covered with sandpaper of #240 and theoptical fiber is wound around the outer periphery of the cylinder withtension of 0.8 N in such a way as to be in contact with the sandpaper is1 dB/km or less.
 4. The optical fiber according to claim 1, wherein aMAC value being a ratio of a mode field diameter MFD [μm] for the lighthaving the wavelength of 1310 nm to a cable cutoff wavelength λcc [nm]is 6.9 or smaller.
 5. The optical fiber according to claim 1, wherein avirtual temperature of glass configuring the glass fiber is 1600° C. orhigher and 1700° C. or lower.
 6. The optical fiber according to claim 1,wherein the core includes a material in which germanium is added to puresilica glass, and the cladding includes the pure silica glass, and hasan absorption peak at a wave number of 2500 cm⁻¹ or larger and 3000 cm⁻¹or smaller in an IR spectrum.
 7. The optical fiber according to claim 1,wherein tensile strength in a center axis direction is larger than 0.69GPa.
 8. The optical fiber according to claim 1, wherein the coatingresin includes a primary coating resin layer covering the outerperiphery of the glass fiber and a secondary coating resin layercovering an outer periphery of the primary coating resin layer.
 9. Theoptical fiber according to claim 8, wherein a Young's modulus of theprimary coating resin layer is 0.7 MPa or smaller, an outer diameter ofthe primary coating resin layer is 120 μm or larger and 140 μm orsmaller, a Young's modulus of the secondary coating resin layer is 800MPa or larger and 3000 MPa or smaller, and an outer diameter of thesecondary coating resin layer is 150 μm or larger and 170 μm or smaller.10. The optical fiber according to claim 9, wherein the coating resinfurther includes a colored resin layer covering an outer periphery ofthe secondary coating resin layer, and an outer diameter of the coloredresin layer is 160 μm or larger and 170 μm or smaller.
 11. The opticalfiber according to claim 8, wherein the secondary coating resin layerincludes coloring ink, and configures an outermost layer of the coatingresin.